where \(\alpha , \beta , g, q, f\)  are functions of \(t\) . Using the scalar potential \(\hat{V}= \hat{g}^{i\bar{\jmath }} \partial _i \hat{W} \partial _{\bar{\jmath }} \hat{ \bar{W}}\)  based on eq. (REF ) the masses of the two complex scalars in the \(\hat{X}, \hat{T}\)  superfields can be computed in the globally supersymmetric case. To find these at small \(t\)  we need to present the dependence of the couplings on \(t\)  as given by the solutions of the ERG equations in [1]}
\(\tilde{\zeta }= {1- e^{-2t}\over 4\alpha ^2} \, , \qquad \tilde{\gamma }= {1- e^{-2t} \over \alpha \beta }\, , \qquad \tilde{f} = {e^{2t} f\over \Lambda ^2\sqrt{\alpha }}\, , \qquad \tilde{g}= {1\over 2\alpha \sqrt{\beta }} \ , \) 
